Reuse & Permissions

It is not necessary to obtain permission to reuse this article or its components as it is available under the terms of the Creative Commons Attribution 4.0 International license. This license permits unrestricted use, distribution, and reproduction in any medium, provided attribution to the author(s) and the published article's title, journal citation, and DOI are maintained. Please note that some figures may have been included with permission from other third parties. It is your responsibility to obtain the proper permission from the rights holder directly for these figures.

Export citation

Export citation

Choose format for download:

Download Citation
  • Open Access

Wigner entropy conjecture and the interference formula in quantum phase space

Zacharie Van Herstraeten1,2 and Nicolas J. Cerf3,1

Phys. Rev. A 112, 062207 – Published 3 December, 2025

DOI: https://doi.org/10.1103/1ftk-dm7l

Abstract

Wigner-positive quantum states have the peculiarity to admit a Wigner function that is a genuine probability distribution over phase space. The Shannon differential entropy of the Wigner function of such states—called Wigner entropy for brevity—emerges as a fundamental information-theoretic measure in phase space and is subject to a conjectured lower bound, reflecting the uncertainty principle. In this work, we prove that this Wigner entropy conjecture holds true for a broad class of Wigner-positive states known as beam-splitter states, which are obtained by evolving a separable state through a balanced beam splitter and then discarding one mode. Our proof relies on known bounds on the p-norms of cross Wigner functions and on the interference formula, which relates the convolution of Wigner functions to the squared modulus of a cross Wigner function. Originally discussed in the context of signal analysis, the interference formula is not commonly used in quantum optics although it unveils a strong symmetry under convolution exhibited by Wigner functions of pure states. We provide here a simple proof of the formula and highlight some of its implications. Finally, we prove an extended conjecture on the Wigner-Rényi entropy of beam-splitter states, albeit in a restricted range for the Rényi parameter α≥1/2.

View figure in article

Physics Subject Headings (PhySH)

Article Text

References (55)

  1. F. Albarelli, M. G. Genoni, M. G. A. Paris, and A. Ferraro, Resource theory of quantum non-Gaussianity and Wigner negativity, Phys. Rev. A 98, 052350 (2018).
  2. U. Chabaud, P.-E. Emeriau, and F. Grosshans, Witnessing Wigner negativity, Quantum 5, 471 (2021).
  3. C. T. Lee, Measure of the nonclassicality of nonclassical states, Phys. Rev. A 44, R2775 (1991).
  4. N. Lütkenhaus and S. M. Barnett, Nonclassical effects in phase space, Phys. Rev. A 51, 3340 (1995).
  5. S. De Bièvre, D. B. Horoshko, G. Patera, and M. I. Kolobov, Measuring nonclassicality of bosonic field quantum states via operator ordering sensitivity, Phys. Rev. Lett. 122, 080402 (2019).
  6. E. Wigner, On the quantum correction for thermodynamic equilibrium, Phys. Rev. 40, 749 (1932).
  7. A. Kenfack and K. Życzkowski, Negativity of the Wigner function as an indicator of non-classicality, J. Opt. B: Quantum Semiclass. Opt. 6, 396 (2004).
  8. A. Mari and J. Eisert, Positive Wigner functions render classical simulation of quantum computation efficient, Phys. Rev. Lett. 109, 230503 (2012).
  9. Strictly speaking, states whose Wigner function does not admit any negativity should be denoted as Wigner-non-negative states (since their Wigner function is ≥0 and may even have zeros), but we prefer denoting them as Wigner-positive states in this paper for brevity.
  10. D. Kastler, The C*-algebras of a free boson field: I. Discussion of the basic facts, Commun. Math. Phys. 1, 14 (1965).
  11. G. Loupias and S. Miracle-Sole, C*-algèbres des systèmes canoniques. I, Commun. Math. Phys. 2, 31 (1966).
  12. G. Loupias and S. Miracle-Sole, C*-algèbres des systèmes canoniques. II, Ann. l'inst. Henri Poincaré A Phys. Théor. 6, 39 (1967).
  13. F. J. Narcowich and R. F. O'Connell, Necessary and sufficient conditions for a phase-space function to be a Wigner distribution, Phys. Rev. A 34, 1 (1986).
  14. H. P. Robertson, The uncertainty principle, Phys. Rev. 34, 163 (1929).
  15. I. Białynicki-Birula and J. Mycielski, Uncertainty relations for information entropy in wave mechanics, Commun. Math. Phys. 44, 129 (1975).
  16. I. Bialynicki-Birula, Rényi entropy and the uncertainty relations, Found. Probab. Phys. 889, 52 (2007).
  17. Z. Van Herstraeten and N. J. Cerf, Quantum Wigner entropy, Phys. Rev. A 104, 042211 (2021).
  18. A. Hertz, M. G. Jabbour, and N. J. Cerf, Entropy-power uncertainty relations: Towards a tight inequality for all Gaussian pure states, J. Phys. A: Math. Theor. 50, 385301 (2017).
  19. Z. Van Herstraeten, M. G. Jabbour, and N. J. Cerf, Continuous majorization in quantum phase space, Quantum 7, 1021 (2023).
  20. N. Cerf, A. Hertz, and Z. Van Herstraeten, Complex-valued Wigner entropy of a quantum state, Quantum Stud.: Math. Found. 11, 331 (2024).
  21. N. C. Dias and J. N. Prata, On a recent conjecture by Z. Van Herstraeten and N. J. Cerf for the quantum Wigner entropy, Ann. Henri Poincaré 24, 2341 (2023).
  22. Q. Qian and C. N. Gagatsos, Wigner non-negative states that verify the Wigner entropy conjecture, Phys. Rev. A 110, 012228 (2024).
  23. A. J. E. M. Janssen, Application of the Wigner distribution to harmonic analysis of generalized stochastic processes, Ph.D. thesis, Technische Hogeschool Eindhoven, 1979.
  24. F. Hlawatsch, Interference terms in the Wigner distribution, Proc. Dig. Sig. Proc. 363 (1984).
  25. E. H. Lieb, Integral bounds for radar ambiguity functions and Wigner distributions, J. Math. Phys. 31, 594 (1990).
  26. A. Royer, Wigner function as the expectation value of a parity operator, Phys. Rev. A 15, 449 (1977).
  27. Note the factor 2 in Eqs. (1) and (2), which originates from our asymmetric conventions, namely â=(x̂+ip̂)/2 but α=x+ip. It implies that the displacement operator D̂(α) shifts the (x,p) coordinates as x↦x+2Re(α) and p↦p+2Im(α). The reason for this choice is that the definition (4) of the Wigner entropy then coincides with its earlier definition in terms of (x,p) coordinates, see Ref. [17].
  28. J. E. Moyal, Quantum mechanics as a statistical theory, Math. Proc. Cambr. Philos. Soc. 45, 99 (1949).
  29. R. L. Hudson, When is the Wigner quasi-probability density non-negative? Rep. Math. Phys. 6, 249 (1974).
  30. J. Garcia-Bondia and J. C. Várilly, Nonnegative mixed states in Weyl-Wigner-Moyal theory, Phys. Lett. A 128, 20 (1988).
  31. T. Bröcker and R. F. Werner, Mixed states with positive Wigner functions, J. Math. Phys. 36, 62 (1995).
  32. A. Mandilara, E. Karpov, and N. J. Cerf, Extending Hudson's theorem to mixed quantum states, Phys. Rev. A 79, 062302 (2009).
  33. A. Lenard, Thermodynamical proof of the Gibbs formula for elementary quantum systems, J. Stat. Phys. 19, 575 (1978).
  34. M. J. Bastiaans, Lower bound in the uncertainty principle for partially coherent light, J. Opt. Soc. Am. 73, 1320 (1983).
  35. J. P. Santos, G. T. Landi, and M. Paternostro, Wigner entropy production rate, Phys. Rev. Lett. 118, 220601 (2017).
  36. M. Brunelli, L. Fusco, R. Landig, W. Wieczorek, J. Hoelscher-Obermaier, G. Landi, F. L. Semião, A. Ferraro, N. Kiesel, T. Donner, G. De Chiara, and M. Paternostro, Experimental determination of irreversible entropy production in out-of-equilibrium mesoscopic quantum systems, Phys. Rev. Lett. 121, 160604 (2018).
  37. G. Adesso, D. Girolami, and A. Serafini, Measuring Gaussian quantum information and correlations using the Rényi entropy of order 2, Phys. Rev. Lett. 109, 190502 (2012).
  38. N. L. Guevara, R. P. Sagar, and R. O. Esquivel, Information uncertainty-type inequalities in atomic systems, J. Chem. Phys. 119, 7030 (2003).
  39. H. G. Laguna and R. P. Sagar, Shannon entropy of the Wigner function and position-momentum correlation in model systems, Int. J. Quantum Inf. 08, 1089 (2010).
  40. S. J. C. Salazar, H. G. Laguna, and R. P. Sagar, Phase-space quantum distributions and information theory, Phys. Rev. A 107, 042417 (2023).
  41. The lower bound ln(2π)+S(ρ̂) depends on the von Neumann entropy S(ρ̂) of state ρ̂ [T. Haas, private communication, 2024].
  42. A. J. E. M. Janssen, Proof of a conjecture on the supports of Wigner distributions, J. Fourier Anal. Appl. 4, 723 (1998).
  43. C. Weedbrook, S. Pirandola, R. García-Patrón, N. J. Cerf, T. C. Ralph, J. H. Shapiro, and S. Lloyd, Gaussian quantum information, Rev. Mod. Phys. 84, 621 (2012).
  44. P. Bertrand, J. P. Doremus, B. Izrar, V. T. Nguyen, and M. R. Feix, Obtaining non-negative quantum mechanical distribution function, Phys. Lett. A 94, 415 (1983).
  45. R. Jagannathan, R. Simon, E. C. G. Sudarshan, and R. Vasudevan, Dynamical maps and nonnegative phase-space distribution functions in quantum mechanics, Phys. Lett. A 120, 161 (1987).
  46. F. J. Narcowich, Conditions for the convolution of two Wigner distributions to be itself a Wigner distribution, J. Math. Phys. 29, 2036 (1988).
  47. Note the discrepancy with the notation used in Ref. [17], where B denotes the subset of states σ̂(ρ̂1,ρ̂2), whereas Bc denotes the closure of its convex hull.
  48. E. H. Lieb, Proof of an entropy conjecture of Wehrl, Commun. Math. Phys. 62, 35 (1978).
  49. E. H. Lieb and J. P. Solovej, Proof of an entropy conjecture for Bloch coherent spin states and its generalizations, Acta Math. 212, 379 (2014).
  50. A. Grossmann, Parity operator and quantization of δ-functions, Commun. Math. Phys. 48, 191 (1976).
  51. V. Potoček and S. M. Barnett, On the exponential form of the displacement operator for different systems, Phys. Scr. 90, 065208 (2015).
  52. A. Janssen, On the locus and spread of pseudo-density functions in the time-frequency plane, Philips J. Res. 37, 79 (1982).
  53. A. Wehrl, On the relation between classical and quantum-mechanical entropy, Rep. Math. Phys. 16, 353 (1979).
  54. V. Giovannetti, S. Guha, S. Lloyd, L. Maccone, and J. H. Shapiro, Minimum output entropy of bosonic channels: A conjecture, Phys. Rev. A 70, 032315 (2004).
  55. V. Giovannetti, R. García-Patrón, N. J. Cerf, and A. S. Holevo, Ultimate classical communication rates of quantum optical channels, Nat. Photon. 8, 796 (2014).

Outline

Information

Sign In to Your Journals Account

Filter

Filter

Article Lookup

Enter a citation